2022ApJ...925...16T


Query : 2022ApJ...925...16T

2022ApJ...925...16T - Astrophys. J., 925, 16-16 (2022/January-3)

Effects of the ΦMeson on the Properties of Hyperon Stars in the Density-dependent Relativistic Mean Field Model.

TU Z.-H. and ZHOU S.-G.

Abstract (from CDS):

The effects of the Φmeson on the properties of hyperon stars are studied systematically in the framework of the density-dependent relativistic mean field (DDRMF) model. The ph meson shifts the hyperon threshold to a higher density and reduces the hyperon fractions in neutron star cores. It also strongly stiffens the equation of state calculated with various DDRMF effective interactions and increases the maximum mass of hyperon stars, but only a few effective interactions survive under the constraints from recent astrophysical observations. In the DDRMF model, the conformal limit of the sound velocity is still in strong tension with the fact that the maximum mass of neutron stars obtained in theoretical calculations reaches about 2 M ☉. Based on different interior composition assumptions, we discuss the possibility of the secondary object of GW190814 as a neutron star. When the ph meson is considered, DD-ME2 and DD-MEX support the possibility that the secondary object of GW190814 is a hyperon star rapidly rotating with Kepler frequency.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Neutron stars - Nuclear astrophysics - Neutron star cores - Compact objects

Simbad objects: 7

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Number of rows : 7
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 PSR J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
2 GrW 190814 GWE 00 55.8 -27 05           ~ 433 0
3 PSR J0348+0432 Psr 03 48 43.6363173480 +04 32 11.461921260           ~ 311 2
4 PSR J0740+6620 Psr 07 40 45.799 +66 20 33.60           ~ 395 0
5 PSR J1210-5226 Psr 12 10 00.88 -52 26 28.4           ~ 230 1
6 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
7 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1

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